posted on 2012-02-06, 00:00authored byAmit Das, Thomas
Michael Scherer, Abhishek Dutta Chowdhury, Shaikh M. Mobin, Wolfgang Kaim, Goutam Kumar Lahiri
The asymmetrical dinuclear complex [(acac)<sub>2</sub>Ru1(μ-abpy)Ru2(Cym)Cl]PF<sub>6</sub> ([<b>2</b>]PF<sub>6</sub>), with acac<sup>–</sup> = acetylacetonato = 2,4-pentanedionato,
abpy = 2,2′-azobis(pyridine), and Cym = <i>p</i>-cymene
=
1-isopropyl-4-methylbenzene, has been obtained from the mononuclear
precursors [Ru(acac)<sub>2</sub>(abpy)] and [Ru(Cym)Cl<sub>2</sub>]<sub>2</sub>. X-ray crystal
structure analysis suggests the oxidation state formulation [(acac)<sub>2</sub>Ru1<sup>III</sup>(μ-abpy<sup>•–</sup>)Ru2<sup>II</sup>(Cym)Cl]<sup>+</sup> for <b>2</b><sup><b>+</b></sup>, with antiferromagnetic coupling
between one Ru<sup>III</sup> center and the radical-anion bridging
ligand (abpy<sup>•–</sup>), based on the N–N
distance of 1.352(3) Å. As appropriate references, the newly
synthesized mononuclear [(abpy)Ru<sup>II</sup>(Cym)Cl]PF<sub>6</sub> ([<b>1</b>]PF<sub>6</sub>) with
an unreduced NN double bond at <i>d</i>(NN) = 1.269(4)
Å
and the symmetrical dinuclear [(acac)<sub>2</sub>Ru<sup>2.5</sup>(μ-abpy<sup>•–</sup>)Ru<sup>2.5</sup>(acac)<sub>2</sub>] with <i>d</i>(NN) = 1.372(4) Å (rac isomer) support the above assignment
for <b>2</b><sup><b>+</b></sup> as an asymmetrical mixed-valent
configuration
bridged by a radical ligand. Reversible one-electron oxidation leads
to a dication, <b>2<sup>2+</sup></b>, with largely metal-centered
spin (EPR: <i>g</i><sub>1</sub> = 2.207, <i>g</i><sub>2</sub> = 2.155, and <i>g</i><sub>3</sub> = 1.929),
and a weak intervalence charge-transfer absorption at 1700 nm, as
observed by spectroelectrochemistry. These results support a description
of <b>2<sup>2+</sup></b> as [(acac)<sub>2</sub>Ru1<sup>III</sup>(μ-abpy<sup>0</sup>)Ru2<sup>II</sup>(Cym)Cl]<sup>2+</sup>.
Density functional
theory (DFT) calculations suggest that the first reduction of [<b>2</b>]PF<sub>6</sub> also involves the bridging ligand, leading
to [(acac)<sub>2</sub>Ru1<sup>III</sup>(μ-abpy<sup>2–</sup>)Ru2<sup>II</sup>(Cym)Cl]
(<b>2</b>). Experimentally, the first reduction of <b>2</b><sup><b>+</b></sup> is not fully reversible, with evidence
for the loss of chloride to form [(acac)<sub>2</sub>Ru1(μ-abpy)Ru2(Cym)]<sup>+</sup> (<b>2a<sup>+</sup></b>; <i>g</i><sub>1</sub> = 2.454, <i>g</i><sub>2</sub> = 2.032, and <i>g</i><sub>3</sub> = 1.947).
Further reduction produces [(acac)<sub>2</sub>Ru1<sup>II</sup>(μ-abpy<sup>2–</sup>)Ru2<sup>II</sup>(Cym)] (<b>2a</b>), which
forms [(acac)<sub>2</sub>Ru1<sup>II</sup>(μ-abpy<sup>2–</sup>)Ru2<sup>I</sup>(Cym)]<sup>−</sup>/[(acac)<sub>2</sub>Ru<sup>II</sup>(μ-abpy<sup>•–</sup>)Ru<sup>0</sup>(Cym)]<sup>−</sup> (<b>2a<sup>–</sup></b>) in yet another
one-electron
step (<i>g</i><sub>1</sub> = 2.052, <i>g</i><sub>2</sub> = 2.008, and <i>g</i><sub>3</sub> = 1.936). The
major electronic transitions for each redox state have been assigned
by time-dependent DFT calculations.